1. B-physics in ATLAS V.Nikolaenko, IHEP on behalf of ATLAS collaboration 1B-physics in ATLAS 20 Nov 2012

2. Outline B-physics triggers Quarkonium production and spectroscopy Measurement of the b-hadron production cross section Measurement of Λ b lifetime and mass Limit on BR(B s →μ + μ - ) CP-violating parameters in B s decays 2B-physics in ATLAS 20 Nov 2012

3. Invariant mass of oppositely charged muon candidate pairs for different triggers at the beginning of 2011 data 3 EF_2mu4_ denotes two muon triggers at level 1, confirmed at the high level trigger, with both objects passing a threshold of 4 GeV EF_mu20 denotes a single muon trigger at level, passing a threshold of 20GeV Jpsimumu, Bmumu, Upsimumu and DiMu denote coarse invariant mass windows, as calculated using the trigger objects The EF_2mu4_DiMu trigger was prescaled for some of the later data taking periods B-physics in ATLAS 20 Nov 2012

4. Trigger and selection requirements Dimuon triggers are the main working tool of the B-Physics group. Many processes of interest have di-lepton final state, or di-lepton plus additional soft object – photon or track(s). At relatively small transverse momenta, dimuons provide significantly better mass resolution and a clean trigger in comparison with electrons. CP-violation and rare decay studies are based on low-p t dimuon triggers. Some studies are based on a single muon triggers. In 2011 run the EF_2mu4 J/ψ and Upsilon triggers had no prescale. With the rise of instantaneous luminosity in 2012, the trigger requirements become significantly tighter. The L1_2mu4 trigger has been prescaled by a factor >10 at L=5.0 x 10 33 and the muon stream data were collected with L1_mu4mu6 or L1_2mu6 triggers. B-physics analyses based mainly on combined muons (reconstructed in Inner detector plus muon spectrometer), with muon transverse momentum greater than 4 GeV and with small impact parameters with respect to the primary vertex. Some analyses use specific triggers with one or two muons in the Barrel, there is a better reconstruction precision and less BG in comparison with Endcaps. Some analyses accept also muons tagged in calorimeters with tracks reconstructed in Inner detector only. The photon in χ b study is reconstructed either through conversion to e + e - or by direct calorimetric measurement, with the ‘‘loose’’ photon selection and a minimum photon transverse energy of 2.5 GeV. Data sample used for this study has been acquired at √s=7 TeV and corresponding to an integrated luminosity of 4.4 fb -1. Final result is obtained with converted photons, with requirements on p t >0.5 GeV for both tracks, a small angle between track, a confirmation of e-hypothesis in TRT and a distance between reconstructed vertex and the beam > 4 cm. 4B-physics in ATLAS 20 Nov 2012

5. Differential cross-sections of inclusive, prompt and non-prompt J/ψ at √s=7 TeV using L=2.3 pb -1 5B-physics in ATLAS 20 Nov 2012

6. Υ(1s) production cross section 6 Results are based on an integrated luminosity of 1.13 pb -1 Both muons have p t μ > 4 GeV and absolute pseudorapidity |η μ | < 2.5 B-physics in ATLAS 20 Nov 2012

7. Upsilon production Measurements of ϒ (1,2,3S) a test of production mechanisms and complementary to J/ψ measurements:  No contributions from B-decays  Heavier quark mass provides better perturbative convergence  More excited states Y(1,2,3S) and χ b (nP) add complication  Larger background contributions, Upsilon states merge together Current analysis uses 1.8 fb -1 of 2011 data ~10 7 ϒ (nS) candidates (background subtracted). Measure inclusive/fiducial production cross-sections as function of ϒ p T in central and forward rapidities, and as p T -integrated rapidity spectra for each of the Upsilon states Also measure production ratios between states vs p T and rapidity 7 ATLAS preliminary B-physics in ATLAS 20 Nov 2012

8. Upsilon cross-section measurements Fiducial cross-section measurements in p T (μ)>4 GeV, |η(μ)|<2.3 Most precise, most differential, widest p T range measurement (uncertainties ~6% on average) Measurement of ϒ (nS) to ϒ (1S) production ratios vs. p T and rapidity NLO pQCD simply predicts these ratios to be 35% and 29% for the ϒ (2S) and ϒ (3S) 8B-physics in ATLAS 20 Nov 2012 ATLAS preliminary

9. Y(1,2S) differential cross sections B-physics in ATLAS 20 Nov 20129 d 2 σ/dp t dy x BR(Yn→μμ)for Y(1S) left, Y(2s) right; at 0<|y|<1.2 (top) and 1.2<|y|<2.4 (bottom) p t range up to 70 GeV Alignment variations in blue; NNLO Color Singlet inclusive in red; Color Evaporation Model in lilac lines This result is much more complete than Tevatron or current CMS results. ATLAS preliminary

10. χ b → (Upsilon(nS)+γ and χ b (3P) discovery End of last year ATLAS discovered new quark-antiquark bound state, the χ bJ (3P). Now has a new entry in the PDG 2012… Discovery now confirmed by LHCb and DØ: ATLAS mass: 10.530±0.005 stat ±0.008 syst GeV LHCb mass: 10.535±0.010 stat ±0.??? syst GeV DØ mass: 10.551±0.014 stat ±0.017 syst GeV ATLAS result remains most precise! Production x-sec and properties measurements ongoing! 10B-physics in ATLAS 20 Nov 2012

11. b-hadron production cross section using decays to D* + μ - X in pp collisions at √s=7 TeV 11 Δm for D* + μ combinations of opposite sign and same sign (dashed) m(D* + μ) for combinations of opposite sign and within ±3σ of the Δm peak Differential cross section for H b production as a function of p t in the fiducial kinematical region p t (H b ) > 9 Gev; |η(H b )|<2.5 Used dataset corresponding to integrated luminosity L=3.3 pb -1, collected during the 2010 LHC run B-physics in ATLAS 20 Nov 2012

12. Measurement of Λ b lifetime and mass 12 Λ b lifetime and mass measured in Λ b →J/ψΛ(pπ) channel: Discrepancies observed between CDF and DØ results (1.8σ difference) in Λ b lifetime Λ 0 vertex efficiency decreases with distance from center of detector – careful study needed to avoid selection biases; Trigger inefficiency depending on the impact parameter of a single muon was studied in details and included in syst. error Use simultaneous mass and lifetime ML fit to extract lifetime: B-physics in ATLAS 20 Nov 2012

13. Measurement of Λ b lifetime and mass 13 Λ b lifetime measurement: ATLAS measures 1.499±0.036±0.017 ps (=±0.040 ps), better than the existing best measurements Λ b mass measurement: ATLAS measures 5619.7±0.7±1.1 compares well with recent LHCb 5919.19±0.7±0.3 it is the second best measurement and reduces the PDG error in the average from 0.7 to 0.6 MeV. B-physics in ATLAS 20 Nov 2012

14. Limit on BR(B s →μ + μ - ) A limit on the branching fraction BR(B s →μ + μ - ) is set using 2.4 fb -1 of integrated luminosity collected in 2011. The process B +- →J/ψK +-, with J/ψ→μ + μ -, is used as a reference channel for the normalization of integrated luminosity, acceptance and efficiency. The final selection is based on a multivariate analysis performed on three categories of events determined according to their mass resolution ( the largest pseudorapidity value of two muons |η max |<1.0, 1.0<|η max |<1.5, 1.5<|η max }<2.5), yielding a limit of BR(B s →μ + μ - ) < 2.2(1.9) x 10 -8 at 95% (90%) Conf. Level. Next step is to double statistics with full 2011 data, but hope to gain more than a ~sqrt(2) improvement on sensitivity due to improvements in the analysis. Comment: in the 2012 data number of events per inverse femtobarn dropping due to trigger conditions, therefore the expected improvement is less than sqrt(lumi). 14B-physics in ATLAS 20 Nov 2012

15. Limit on BR(B s →μ + μ - ) 15 Invariant mass distribution of candidates in data. For each mass-resolution category (top to bottom) each plot shows the invariant mass distribution for the selected candidates in data (dots), the signal (continuous line) as predicted by MC assuming BR(B s 0 -> μ + μ - ) = 3.5 x 10−8, and two dashed vertical lines corresponding to the optimized Delta_m cut. The grey areas correspond to the sidebands used in the analysis B-physics in ATLAS 20 Nov 2012

16. Limit on BR(B s →μ + μ - ) 16 Observed CLs (circles) as a function of BR(B s ->μ + μ - ). The 95% CL limit is indicated by the horizontal (red) line. The dark (green) and light (yellow) bands correspond to ±1sigma and ±2sigma fluctuations on the expectation (dashed line), based on the number of observed events in the signal and sideband regions Note: LHCb just has submitted a paper based on 2011 + a half of 2012 statistics and got a BR value well consistent with SM prediction and with precision close to 3σ. B-physics in ATLAS 20 Nov 2012

17. Physics of J/ψφ decay There is “LHC Gold” B-cannel, new physics can increase SM predicted CP- violation This decay proceeds in S, P and D-waves, leading to CP-even final state in S and D-waves and to CP-odd state in P-wave decay. CP violation arises from interference of B s →J/ψφ decay and B s –antiB s mixing (see next slide) and is proportional to a phase difference, φ s, of the two complex weak amplitudes SM predicted value is small φ s =0.0363±0.0017 rad, currently not accessible by any experiment, however it is within LHC potential Many New physics models predict extra contributions to φ s. Searches started at Tevatron, continue at LHC. φ s is extracted from B s →J/ψφ data by time-dependent angular analysis with 7 unknown parameters B-physics in ATLAS 20 Nov 201217

18. B s mixing B-physics in ATLAS 20 Nov 201218

19. Method of CP-measurement in B s →J/ψφ Final state J/ψφ is a mixture of CP-even (~75%) and CP-odd (~25%) states Three angular momentum states of J/ψφ L=0 S-wave CP-even L=1 P-wave CP-odd L=2 D-wave CP-even φ s can only be measured if CP-states separated using angular distributions of final state particles (used two polar decay angles in J/ψ and φ rest frames and an azimuth angle between two decay planes) 4 additional parameters (strong helicity amplitudes) should be determined simultaneously with the weak parameters 7 parameters in total: Weak: φ s, ΔΓ=(Γ H –Γ L ), Γ=(Γ H +Γ L )/2; Strong: two phases and two absolute values ( 4 independent parameters of three helicity amplitudes). Without tagging and for small φ s, one of the strong phase (φ perp in the transversity notation) cannot be well measured, so the value measured by LHCb used for this quantity. The other phases are measured by ATLAS. B-physics in ATLAS 20 Nov 201219

20. CP violation in B s →J/ψφ(1020) decays 20 Performed a measurement of CP violation in B s → J/ψφ using untagged time-angular analysis of 4.9 fb -1 data collected in 2011 Untagged analysis: decay time distribution and angular correlation between muons and kaons in final state provide information on CP=±1 amplitudes and their interference. Large sample of events: 23 k reconstructed B s from 2011 data sample. B-physics in ATLAS 20 Nov 2012

21. Parameters of CP violation in B s →J/ψφ decay 21 Several parameters describing the B s system are measured: the mean B s lifetime (1/Γ s ), decay width difference ∆Γ s, transversity amplitudes |A 0 (0)|, |A || (0)| and weak phase φ s. The results are consistent with the world average values and with theoretical expectations, in particular φ s = 0.22±0.41±0.10 rad is within 1σ of the expected value in SM. ∆ Γ s = 0.053 ±0.021 stat ± 0.010 syst ps -1 Precision of ∆Γ s and Γ s are competitive with LHCb. Γ s = 0.677 ±0.007 stat ± 0.004 syst ps -1 Next steps: tagged analysis; add 2012 data B-physics in ATLAS 20 Nov 2012

22. Conclusions B-physics at LHC is rich, and ATLAS experiment has produced competitive results in several fields, including spectroscopy, lifetime measurements and untagged analysis of CP-violation in B s decays. Work on the B-tagging methods in ATLAS is ongoing. Many other analyses which were not mentioned in this talk are in progress, for example the ψ(2s) production, associated production of W-boson plus J/ψ, X(3772) study, B +- cross section measurement, B c study. 22B-physics in ATLAS 20 Nov 2012

23. References Measurement of the differential cross-sections of inclusive, prompt and non-prompt J/ψ production in pp collisions at √s = 7 TeV, NP B850 (2011) 387; Υ(1S) Fiducial Production Cross-Section in pp collisions at √s = 7 TeV in ATLAS, PL B705 (2011) 9; Observation of a new χ b state in radiative transitions to Υ(1S) and Υ(2S) at ATLAS, G.Aad et al., Phys.Rev.Lett. 108 (2012) 152001; Search for the decay B 0 s →μ + μ - with the ATLAS detector, G.Aad et al., PL B713, (2012) 387; Measurement of the b-hadron production cross section using decays to D* + μ - X final states in pp-collisions at √s = 7 TeV with the ATLAS detector, G.Aad et al., Nucl. Phys. B 864 (2012) 341; Measurement of the Λ b lifetime and mass in the ATLAS experiment, G.Aad et al., arXiv:1207.2284 [hep-ex], submitted to Phys. Rev. D; φ s and ΔΓ s from time dependent angular analysis of the decay Bs s →J/ψφ by ATLAS, G.Aad et al., arXiv:1208.0572 [hep-ex], submitted to J.High Energy Phys.; Search for the rare decays B->μμ at the LHC with the ATLAS, CMS and LHCb experiments, ATLAS-CONF-2012-061; Measurement of Upsilon production in 7 TeV pp collisions at ATLAS, CERN-PH-EP- 2012-295 ; Combined LHC limit to the decay B s 0 →μμ (ATLAS-CMS-LHCb note) ATLAS-CONF-2012- 061 23B-physics in ATLAS 20 Nov 2012

24. χ b → 24B-physics in ATLAS 20 Nov 2012